F. Nabais - Vilamoura - November 2004 Internal kink mode stability in the presence of ICRH driven fast ions populations F. Nabais, D. Borba, M. Mantsinen,

Slides:



Advertisements
Similar presentations
Progress and Plans on Magnetic Reconnection for CMSO For NSF Site-Visit for CMSO May1-2, Experimental progress [M. Yamada] -Findings on two-fluid.
Advertisements

Ion Heating and Velocity Fluctuation Measurements in MST Sanjay Gangadhara, Darren Craig, David Ennis, Gennady Fiskel and the MST team University of Wisconsin-Madison.
Short wavelength ion temperature gradient driven instability in toroidal plasmas Zhe Gao, a) H. Sanuki, b) K. Itoh b) and J. Q. Dong c) a) Department of.
Particle acceleration in a turbulent electric field produced by 3D reconnection Marco Onofri University of Thessaloniki.
Lecture Series in Energetic Particle Physics of Fusion Plasmas Guoyong Fu Princeton Plasma Physics Laboratory Princeton University Princeton, NJ 08543,
A Kinetic-Fluid Model for Studying Thermal and Fast Particle Kinetic Effects on MHD Instabilities C. Z. Cheng, N. Gorelenkov and E. Belova Princeton Plasma.
6 th ITPA MHD Topical Group Meeting combined with W60 IEA Workshop on Burning Plasmas Session II MHD Stability and Fast Particle Confinement General scope.
Cyclic MHD Instabilities Hartmut Zohm MPI für Plasmaphysik, EURATOM Association Seminar talk at the ‚Advanced Course‘ of EU PhD Network, Garching, September.
William Daughton Plasma Physics Group, X-1 Los Alamos National Laboratory Presented at: Second Workshop on Thin Current Sheets University of Maryland April.
Kinetic Theories of Geodesic Acoustic Modes in Toroidal Plasmas Zhiyong Qiu, F. Zonca and L. Chen IFTS, May 2010.
INTRODUCTION OF WAVE-PARTICLE RESONANCE IN TOKAMAKS J.Q. Dong Southwestern Institute of Physics Chengdu, China International School on Plasma Turbulence.
Fast ion effects on fishbones and n=1 kinks in JET simulated by a non-perturbative NOVA-KN code TH/5-2Rb N.N. Gorelenkov 1), C.Z.Cheng 1), V.G. Kiptily.
TH/3-1Ra Nonperturbative Effects of Energetic Ions on Alfvén Eigenmodes by Y. Todo et al. EX/5-4Rb Configuration Dependence of Energetic Ion Driven Alfven.
D. Borba 1 21 st IAEA Fusion Energy Conference, Chengdu China 21 st October 2006 Excitation of Alfvén eigenmodes with sub-Alfvénic neutral beam ions in.
T. Hellsten IEA Burning Plasma Workshop, July 2005 Tarragona Spain Integrated Modelling of ICRH and AE Dynamics T. Hellsten, T. Bergkvist, T. Johnson and.
Computer simulations of fast frequency sweeping mode in JT-60U and fishbone instability Y. Todo (NIFS) Y. Shiozaki (Graduate Univ. Advanced Studies) K.
1 ST workshop 2005 Numerical modeling and experimental study of ICR heating in the spherical tokamak Globus-M O.N.Shcherbinin, F.V.Chernyshev, V.V.Dyachenko,
Nonlinear Frequency Chirping of Alfven Eigenmode in Toroidal Plasmas Huasen Zhang 1,2 1 Fusion Simulation Center, Peking University, Beijing , China.
6 th Japan-Korea Workshop on Theory and Simulation of Magnetic Fusion Plasmas Hyunsun Han, G. Park, Sumin Yi, and J.Y. Kim 3D MHD SIMULATIONS.
Kinetic Effects on the Linear and Nonlinear Stability Properties of Field- Reversed Configurations E. V. Belova PPPL 2003 APS DPP Meeting, October 2003.
Overview of MHD and extended MHD simulations of fusion plasmas Guo-Yong Fu Princeton Plasma Physics Laboratory Princeton, New Jersey, USA Workshop on ITER.
Hybrid Simulations of Energetic Particle-driven Instabilities in Toroidal Plasmas Guo-Yong Fu In collaboration with J. Breslau, J. Chen, E. Fredrickson,
Particle Distribution Modification by TAE mode and Resonant Particle Orbits POSTECH 1, NFRI 1,2 M.H.Woo 1, C.M.Ryu 1, T.N.Rhee 1,,2.
Excitation of ion temperature gradient and trapped electron modes in HL-2A tokamak The 3 th Annual Workshop on Fusion Simulation and Theory, Hefei, March.
Numerical Simulation on Flow Generated Resistive Wall Mode Shaoyan Cui (1,2), Xiaogang Wang (1), Yue Liu (1), Bo Yu (2) 1.State Key Laboratory of Materials.
HAGIS Code Lynton Appel … on behalf of Simon Pinches and the HAGIS users CCFE is the fusion research arm of the United Kingdom Atomic Energy Authority.
O. Sauter Effects of plasma shaping on MHD and electron heat conductivity; impact on alpha electron heating O. Sauter for the TCV team Ecole Polytechnique.
Chalmers University of Technology Szczecin, 23 March 2006 Meeting with Dr. B. Green Dr. B. Green (Euratom) and Prof. A. Gałkowski (Association Euratom-IPPLM)
Modeling Beam Ion Relaxation with application to DIII-D K.Ghantous, N.N. Gorelenkov PPPL, 2012.
CCFE is the fusion research arm of the United Kingdom Atomic Energy Authority Internal Transport Barriers and Improved Confinement in Tokamaks (Three possible.
Stability Properties of Field-Reversed Configurations (FRC) E. V. Belova PPPL 2003 International Sherwood Fusion Theory Conference Corpus Christi, TX,
Dynamics of ITG driven turbulence in the presence of a large spatial scale vortex flow Zheng-Xiong Wang, 1 J. Q. Li, 1 J. Q. Dong, 2 and Y. Kishimoto 1.
DIII-D SHOT #87009 Observes a Plasma Disruption During Neutral Beam Heating At High Plasma Beta Callen et.al, Phys. Plasmas 6, 2963 (1999) Rapid loss of.
2 The Neutral Particle Analyzer (NPA) on NSTX Scans Horizontally Over a Wide Range of Tangency Angles Covers Thermal ( keV) and Energetic Ion.
Comparison of Ion Thermal Transport From GLF23 and Weiland Models Under ITER Conditions A. H. Kritz 1 Christopher M. Wolfe 1 F. Halpern 1, G. Bateman 1,
NSTX APS DPP 2008 – RWM Stabilization in NSTX (Berkery)November 19, Resistive Wall Mode stabilization in NSTX may be explained by kinetic theory.
Excitation of internal kink mode by barely trapped suprathermal electrons* Youwen Sun, Baonian Wan, Shaojie Wang, Deng Zhou, Liqun Hu and Biao Shen * Sun.
M. Onofri, F. Malara, P. Veltri Compressible magnetohydrodynamics simulations of the RFP with anisotropic thermal conductivity Dipartimento di Fisica,
Lecture Series in Energetic Particle Physics of Fusion Plasmas Guoyong Fu Princeton Plasma Physics Laboratory Princeton University Princeton, NJ 08543,
Kinetic MHD Simulation in Tokamaks H. Naitou, J.-N. Leboeuf †, H. Nagahara, T. Kobayashi, M. Yagi ‡, T. Matsumoto*, S. Tokuda* Joint Meeting of US-Japan.
S. Coda, MHD workshop, PPPL, 22 Nov Advances in sawtooth control for NTM prevention in JET S. Coda 1, L.-G. Eriksson 2, J. Graves 1, R. Koslowski.
STUDIES OF NONLINEAR RESISTIVE AND EXTENDED MHD IN ADVANCED TOKAMAKS USING THE NIMROD CODE D. D. Schnack*, T. A. Gianakon**, S. E. Kruger*, and A. Tarditi*
Influence of pressure-gradient and average- shear on ballooning stability semi-analytic expression for ballooning growth rate S.R.Hudson 1, C.C.Hegna 2,
RFX workshop / /Valentin Igochine Page 1 Control of MHD instabilities. Similarities and differences between tokamak and RFP V. Igochine, T. Bolzonella,
1 A Proposal for a SWIM Slow-MHD 3D Coupled Calculation of the Sawtooth Cycle in the Presence of Energetic Particles Josh Breslau Guo-Yong Fu S. C. Jardin.
The influence of non-resonant perturbation fields: Modelling results and Proposals for TEXTOR experiments S. Günter, V. Igochine, K. Lackner, Q. Yu IPP.
Chernoshtanov I.S., Tsidulko Yu.A.
NIMROD Simulations of a DIII-D Plasma Disruption
Summary of IAEA Theory Papers on Energetic Particle Physics Guoyong Fu.
Simulations of NBI-driven Global Alfven Eigenmodes in NSTX E. V. Belova, N. N. Gorelenkov, C. Z. Cheng (PPPL) NSTX Results Forum, PPPL July 2006 Motivation:
1 Magnetic components existing in geodesic acoustic modes Deng Zhou Institute of Plasma Physics, Chinese Academy of Sciences.
Neoclassical Effects in the Theory of Magnetic Islands: Neoclassical Tearing Modes and more A. Smolyakov* University of Saskatchewan, Saskatoon, Canada,
Helically Symmetry Configuration Evidence for Alfvénic Fluctuations in Quasi-Helically Symmetric HSX Plasmas C. Deng and D.L. Brower, University of California,
T. Hellsten IAEA TM Meeting on Energetic Particles, San Diego 2003 T. Hellsten 1, T. Bergkvist 1, T.Johnson 1, M. Laxåback 1 and L.-G. Eriksson 2 1 Euratom-VR.
Simulations of Energetic Particle Modes In Spherical Torus G.Y. Fu, J. Breslau, J. Chen, E. Fredrickson, S. Jardin, W. Park Princeton Plasma Physics Laboratory.
Nonlinear Simulations of Energetic Particle-driven Modes in Tokamaks Guoyong Fu Princeton Plasma Physics Laboratory Princeton, NJ, USA In collaboration.
1 ASIPP Sawtooth Stabilization by Barely Trapped Energetic Electrons Produced by ECRH Zhou Deng, Wang Shaojie, Zhang Cheng Institute of Plasma Physics,
Energetic Particles Interaction with the Non-resonant Internal Kink in Spherical Tokamaks Feng Wang*, G.Y. Fu**, J.A. Breslau**, E.D. Fredrickson**, J.Y.
Resistive Modes in CDX-U J. Breslau, W. Park. S. Jardin, R. Kaita – PPPL D. Schnack, S. Kruger – SAIC APS-DPP Annual Meeting Albuquerque, NM October 30,
TH/7-1Multi-phase Simulation of Alfvén Eigenmodes and Fast Ion Distribution Flattening in DIII-D Experiment Y. Todo (NIFS, SOKENDAI) M. A. Van Zeeland.
Energetic ion excited long-lasting “sword” modes in tokamak plasmas with low magnetic shear Speaker:RuiBin Zhang Advisor:Xiaogang Wang School of Physics,
U NIVERSITY OF S CIENCE AND T ECHNOLOGY OF C HINA Influence of ion orbit width on threshold of neoclassical tearing modes Huishan Cai 1, Ding Li 2, Jintao.
Reconnection Process in Sawtooth Crash in the Core of Tokamak Plasmas Hyeon K. Park Ulsan National Institute of Science and Technology, Ulsan, Korea National.
Kinetic Effects on Slowly Rotating Magnetic Islands in Tokamaks
Huishan Cai, Jintao Cao, Ding Li
8th IAEA Technical Meeting on
Recent work on the control of MHD instabilities at
Influence of energetic ions on neoclassical tearing modes
Stabilization of m/n=1/1 fishbone by ECRH
20th IAEA Fusion Energy Conference,
Presentation transcript:

F. Nabais - Vilamoura - November 2004 Internal kink mode stability in the presence of ICRH driven fast ions populations F. Nabais, D. Borba, M. Mantsinen, M.F. Nave, S. Sharapov and JET-EFDA contributors

F. Nabais - Vilamoura - November 2004 Outline Internal kink mode n=1, m=1 Effect of ICRH driven populations on Perturbative method Variational method Quantitative results (F. Porcelli et al. Phys. Plasmas,1 (3), 470 (1994)) Sawteeth Fishbones Sawteeth, (R. White et al. Phys. Fluids B 2, 745 (1990)) Qualitative results MHD energy functional Fast ions energy functional Fast ions Objective : Explain experimental observations in JET

F. Nabais - Vilamoura - November 2004 Perturbative method eigenfunction perturbation (F. Porcelli et al. Phys. Plasmas,1 (3), 470 (1994)) Relevant equations, which include Finite Orbit Width effects, Adiabatic part - destabilizing

F. Nabais - Vilamoura - November 2004 Perturbative method CASTOR-K Non-adiabatic part - stabilizing Sawteeth Safety factor on axis Fast ions temperature Location of the ICRH resonant layer Fast ions radial profile

F. Nabais - Vilamoura - November 2004 Non-adiabatic Adiabatic part of (Preliminar results) Destabilizing increases with T HOT Effect of the ICRH fast ions on sawteeth Blue regions: stabilizing Red regions: destabilizing as function of q 0 and T HOT on-axis heating

F. Nabais - Vilamoura - November 2004 Experiments with low plasma densities T HOT ~ P ICRH nene Sawteeth destabilization occurred when:  ICRH power increases  Plasma density decreases Application to experiments Non-adiabatic as function of T HOT

F. Nabais - Vilamoura - November 2004  The stabilizing effect of the non-adiabatic part of decreases as T HOT increases, so this mechanism for sawtooth stabilization is weakened.  The destabilizing effect associated with the adiabatic part of is increased. Numerical results show: Application to experiments  The non-adiabatic part of is dominant.  Sawteeth destabilization coincides with an increase in T HOT

F. Nabais - Vilamoura - November 2004 Variational method Solutions of the internal kink dispersion relation: Low frequency High frequency Kink Branch Ion Branch Fishbone Branch Sawteeth Low frequency (diamagnetic) fishbones High frequency (precessional) fishbones (R. White et al. Phys. Fluids B 2, 745 (1990)) (B. Coppi and F. Porcelli P. R.L, 57, 2272 (1986)) ω ≈ ω *i ω ≈ (L. Chen et. al P. R.L, 52, 1122 (1984)) (Ideal limit)

F. Nabais - Vilamoura - November 2004 Marginal equation ω=real, ideal limit, ICRH population Stability governed mainly by Ideal (MHD) growth rate Diamagnetic frequency Fast particles beta Determination of the regions of stability

F. Nabais - Vilamoura - November 2004 I I hh Regions of stability

F. Nabais - Vilamoura - November 2004 Magnetic spectrogram from JET Precessional Fishbones Diamagnetic Fishbones Hybrid Fishbones Sawtooth Crash

F. Nabais - Vilamoura - November 2004 Increases Decreases during a burst Increases between bursts In between crashes the q=1 surface expands In between crashes the ion bulk profile peaks : 3 kHz20 kHz Variation of the relevant parameters

F. Nabais - Vilamoura - November 2004 Variation of the regions of stability hh I I

F. Nabais - Vilamoura - November 2004 Regions of stability I I hh

F. Nabais - Vilamoura - November 2004 Ion branch Fishbone branch β h decreases during the burst Diamagnetic behaviour Precessional behaviour Coalescent Ion-Fishbone branch hh  (R. White et al. Phys. Fluids B 2, 745 (1990)) Solutions of the dispersion relation ω *i2 ω *i1 ω *i1 < ω *i2

F. Nabais - Vilamoura - November 2004 Time (s) Magnetic perturbation Magnetic perturbation for an hybrid fishbone

F. Nabais - Vilamoura - November 2004 Ion mode Fishbone mode Coalescent ion-fishbone mode Low frequency fishbones High frequency fishbones Hybrid fishbones Both types of fishbones occuring simultaneously ( Gorolenkov et al. “Fast ions effects on fishbones and n=1 kinks in JET simulated by a non-perturbative NOVA-KN code, this conference) Modes and regimes

F. Nabais - Vilamoura - November 2004 Summary Perturbative Method - Accurate calculation of  HOT for a realistic geometry - Only for the “kink mode” Variational Method - All branches of the dispersion relation - Simplified geometry and fast ions’ distribution function, suitable only for a qualitative approach - Predicts changes in instabilities behaviour knowing the relevant parameters Stabilizing term vanishes for high fast ions temperatures Hybrid fishbones and both types of fishbones occuring simultaneously